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Bindings: Python
Note: PyO3 May not build correctly on MacOS. See Issue #143
First, the Python bindings require the following Python3 modules to be installed:
setuptools_rust
testresources
-
rustc
, must be available on your system PATH. - On Windows machines, you may need to install the Visual Studio C++ Build Tools.
Running:
python3 -m pip install .
Will compile RustBCA as a library, construct the Python bindings, and build a python module, libRustBCA.pybca, that can be immediately imported into any Python script. An annotated example, test_rustbca.py, is included in the examples folder.
examples/test_rustbca.py
uses simple_bca_list_py()
to simulate 1 keV helium on tungsten. To run, you need the Python bindings installed (see above), matplotlib, and numpy. It compares the sputtering yield to Yamamura's formula and the reflection coefficient to Thomas' formula. Differences between RustBCA simulation results and these formulas at moderate energy should be within 10% for most materials; it also produces the sputtered energy distribution and the implanted depth distribution using matplotlib, displayed below.
To run the example, simply call the script from the command line:
C:\rustbca>python examples\test_rustbca.py
or
username@PCNAME:/rustbca$python3 examples/test_rustbca.py
Sample output of test_rustbca.py looks like this:
Running RustBCA for 100000 He ions on W at 1.0 keV...
This may take several minutes.
Simulation complete. Processing data...
Data processing complete.
RustBCA Y: 0.0287 Yamamura Y: 0.025479590898842535
RustBCA R: 0.50558 Thomas R: 0.4780755087527244
Time per ion: 1.192930190563202 us/He
Implanted helium on tungsten at 1 keV
Energy distribution of tungsten sputtered by helium at 1 keV
simple_bca_py
and simple_bca_list_py
can be used for simple targets (that is, targets made of one species instead of compound targets).
-
x, y, z
: starting position in angstroms (Recommended: 0, 0, 0); Note: not used for simple_bca_list_py -
ux, uy, uz
: initial direction(s); Note: ux cannot be exactly 0 due to gimbal lock. -
E
: energy/energies in eV -
Z1
: atomic number(s) of incident ion(s) -
M1
: atomic mass(es) of incident ion(s) (amu) -
Ec1
: cutoff energy/energies of incident ion (eV) -
Es1
: surface binding energy/energies of incident ion (eV) -
Z2
: atomic number of material -
M2
: atomic mass of material (amu) -
Ec2
: cutoff energyof material (eV) -
Es2
: surface binding energyof material (eV) -
n2
: number density of material (1/angstrom^3) -
Eb2
: bulk binding energy of material (eV)
The output of simple_bca_list_py
is a list of output particles with the following parameters:
[[Z, m (amu), E (eV) x (Angstrom), y (Angstrom), z (Angstrom), ux, uy, uz], ...]
Note that this includes implanted particles (with E < Es & x > 0), reflected particles (with E > 0 & x < 0), and sputtered particles (Z = Z_target & x < 0 & E > 0). See examples/test_rustbca.py
for an example of filtering the output for implanted, reflected, and sputtered particles.
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